The symmetry of the first excited state of one of the normal modes in is . Based on the character table for the point group given below, the symmetry of the second excited state for this mode in terms of the irreducible representations is:

C2v E C2 σv(xz) σ'v(yz)
A1 1 1 1 1
A2 1 1 -1 -1
B1 1 -1 1 -1
B2 1 -1 -1 1

1
2A1+B1
2
A1​ AB2
3
A2B1
4
2AB2

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